Method of making a silicon integrated circuit waveguide

ABSTRACT

A method for forming a semiconductor waveguide includes forming a layer of expitaxial silicon (12) over a substrate (10). The impurity concentration of the layer (12) is higher than that of the substrate (10). A second layer (14) of epitaxial silicon is disposed over the upper surface of the layer (12) with a higher resistivity than that of the substrate (10). A masking layer (16) is then disposed over the substrate and then patterned, and then the layer (14) selectively etched down to the upper surface of the layer (12). The layer (12)) is then porified to form an insulating layer (12&#39;) from the layer (12). The porous film is then converted by oxidation to a silicon dioxide layer (13). The sidewalls of the resulting ridge (14) are then oxidized to form sidewall layers (13&#39;) and then the masking layer (16) removed from the upper layer. The upper surface of ridge (14) is oxidized to form an upper insulating layer to extend the sidewall layer (13&#39;) over the entire upper surface and sidewalls of the ridge (14). A layer (18) of insulating material is then disposed over the substrate.

RELATED APPLICATIONS

This is a continuation of application Ser. No. 07/326,104 filed Mar. 20,1989 and entitled "INTEGRATED CIRCUIT WAVEGUIDE", now U.S. Pat. No.4,927,781.

TECHNICAL FIELD OF THE INVENTION

The present invention pertains in general to integrated optics, and moreparticularly, to a waveguide fabricated utilizing integrated optictechnology.

BACKGROUND OF THE INVENTION

As integrated optics has developed, the use of various componentsperipherally related with such things as integrated lasers, switches,etc. has also developed. One of the most important peripheral elementsis waveguide interconnects. Although optical fibers are utilized forlong transmission lengths to interconnect various locations due to theirminimum transmissive power loss, these would be classified as discreteelements and are impractical for an integrated circuit relating tooptics.

While it has long been useful to fabricate integrated optic waveguidesfrom other materials disposed on silicon, using its superior mechanicalproperties, it has become practical to fabricate the waveguides fromsilicon itself. In recent years, the efforts of the telecommunicationsindustry to minimize dispersive power loss in fibers have driven carrierwavelengths further into the infrared spectrum. Presently, the commonlyused wavelengths are 1.3 um and 1.55 um. Consequently, the need hasarisen for integrated optical devices to operate at long wavelengths aswell. Silicon itself is transparent in the 1.2-6.0 micrometer wavelengthrange and therefore provides some advantages as integrated waveguides inthat it behaves as a low loss dielectric in its single crystalline,semi-insulating state, i.e., low-doped. Integrated waveguides aretypically fabricated from dielectric slabs or channels that are clad orbounded by dielectrics with lower indices of refraction. This allows thelight to propagate within the waveguide with very little attenuation dueto the confinement of the light waves by total internal reflection.Silicon with its index of refraction of approximately 3.5 at awavelength of 1.3 micrometer will form a waveguide when clad by silicondioxide, which has an index of refraction of approximately 1.5.

One of the primary problems with disposing silicon dioxide about asilicon waveguide is the accessibility to the silicon surfaces duringprocessing. In one process wherein the surfaces are accessible from topside processing, ridge structures are etched with or without subsequentback fill. This results in roughness due to etching process which leadsto scattering losses when light reflects from the ridge walls. Further,this process utilizes air on the exterior with an index of refraction of1.0 as compared to the index of refraction for silicon of 3.5, resultingin a large refractive index difference, and further enhancing scatteringloss.

In another top side process, the ridge structures are etched and then alayer of thermal oxide formed on the etched surfaces. This provides someimprovement in that the silicon dioxide has a higher refractive index ascompared to air and the surface roughness is smoothed out by theoxidation reaction. Further, this silicon dioxide/silicon interfaceformed by the thermal oxidation tends to have silicon-rich transitionlayers near the boundary, resulting in a graded index profile.

Other processes for fabricating semiconductor waveguides are directedtoward surfaces which are not accessible to top side processing, i.e.,the undersides of the channels. In one process, a heavily dopedsubstrate is utilized with the ridge waveguide formed on the uppersurface thereof. This is illustrated in R. A. Soref et al., "SiliconGuided-Wave Optics", Solid State Technology, Nov. 1988, page 95. Oneproblem with this type of structure is that the refractive indexdifference is very small such that a large fraction of transmitted poweris actually carried in the heavily doped region if the waveguide aboveit is sufficiently thin. Heavily doped silicon, however, is a veryabsorptive material resulting in significant light attenuation.

Another structure for processing the underside of the waveguide utilizesthe underlying layer of silicon dioxide with silicon deposited on theupper surface thereof. With this type of process, it is necessary tofabricate defect free monocrystalline silicon layers. Any degree ofdefectiveness or polycrystallinity will drastically increase absorption.This is typically referred to as silicon on insulator (SOI) technology.

Another type of SOI technology requires the formation of buried silicondioxide by high energy implantation of oxygen ions through singlecrystal silicon, followed by high temperature annealing. This isreferred to as the SIMOX process in Kurdi and Hall, "Optical Waveguidesin Oxygen-Implanted Buried-Oxide Silicon-On-Insulator Structure", OpticsLetters, Feb. 1988, volume 13, number 2, page 175. The problems withthis type of system are the complexity and the size of the high energyimplanters, residual damage in the silicon, and stress and deformationbrought about by several factors, including volumetric expansion fromthe implanted oxygen, volumetric expansion from the subsequentsilicon-to-silicon dioxide transition, and the extremely hightemperature required for the transition.

SUMMARY OF THE INVENTION

The present invention disclosed and claimed herein comprises a methodfor fabricating a semiconductor waveguide. The waveguide is fabricatedby first providing a semiconductor substrate having a low doping level.A first layer of semiconductor material is formed over the surface ofthe substrate and doped to a higher concentration than the substrate. Asecond layer of semiconductor material is then disposed over the surfaceof the first layer with a lower concentration of dopant materials andthe masking layer is disposed on the upper surface of at least oneridge. The second layer of semiconductor material is then patterned andselectively etched down to the upper surface of the first layer ofsemiconductor material to define at least one ridge. The first layer ofsemiconductor material is then porified and oxidized to form aninsulating layer underneath at least one ridge. Insulating sidewalllayers are formed on the substantially vertical surface of the at leastone ridge and the masking layer removed. An insulating layer is thenformed over the upper surface of the at least one ridge.

BRIEF DESCRIPTION OF THE DRAWINGS

For a more complete understanding of the present invention andadvantages thereof, reference is now made to the following descriptiontaken in conjunction with the accompanying Drawings in which:

FIG. 1 illustrates a cross-sectional diagram of a substrate with twoepitaxial layers, an anodizable and a low-doped top layer;

FIG. 2 illustrates the structure of FIG. 1 with a masking pattern;

FIG. 3 illustrates the structure of FIG. 2 after etching of the toplayer to form ridged channels;

FIG. 4 illustrates the structure of FIG. 3 after the structure has beenanodized;

FIG. 5 illustrates the structure of FIG. 4 after converting of theporous film by oxidation and forming of side wall oxide layers;

FIG. 5a illustrates the structure of FIG. 5 after removing the maskingmaterial and formation of a top oxide layer;

FIG. 6 illustrates the structure of FIG. 5 after a dielectric back fill;and

FIG. 7 illustrates a perspective view of the structure of FIG. 6.

DETAILED DESCRIPTION OF THE INVENTION

Referring now to FIG. 1, there is illustrated a cross-sectional diagramof a semiconductor substrate 10. The semiconductor substrate 10 iscomprised of an intrinsically doped silicon doped to conventionallevels. The surface of the substrate is covered with an expitaxial layer12 and an epitaxial layer 14. The expitaxial layer 12 is typicallyformed after cleaning the starting substrate and which can be an N-typesubstrate in the 2-4 Ohm-cm range and then immediately thereaftergrowing an N-plus epitaxial (epi) layer doped in the range of 10¹⁸ cm⁻³to 10¹⁹ cm⁻³ to a predetermined thickness. This results in the layer 12which serves as an anodizable layer with a resistivity and thicknessutilized to set the final porosity of the anodized film and the finalthickness of an isolation oxide, respectively. The second layer 14 is anN-type epilayer that is grown with a higher resistivity in the 10-100Om-cm region to provide the structure in FIG. 1.

Referring now to FIG. 2, after forming the epilayers 12 and 14, a layerof masking material is disposed over the substrate and then patternedusing photolithographic techniques well known in the art, to formmasking regions 16. The masking structure is composed to act as aselective etch mask, an anodization mask, and an oxidation mask. Abilayer of chemical vapor deposited silicon oxide on top of LPCVDsilicon nitride can be used for this purpose. Each of the maskingregions 16 defines a waveguide structure. This structure is then etchedas illustrated in FIG. 3 to etch only the upper epilayer 14 and leavethe lower epilayer 12 untouched. This is a selective etch processwhereby the resulting walls are vertical or nearly vertical. Theresulting ridge channels are defined by the masking layer 16, and theridge cross section is essentially rectangular, where the width can bechosen to be any value from that of the thickness of layer 14 to muchlarger. It is shown in the Figure that a portion of the masking layer 16thickness is consumed in the RIE process. In another embodiment, thevertical etching is carried out partially through or completely throughthe layer 12.

As illustrated in FIG. 4, after definition of the ridge channel 14', thelayer 12 is then anodized to form a layer 12'. The desired porosity of50%-60% is achieved by subjecting the substrate to HF acid in aconcentration that varies between 10% by weight up to 40% by weight withcurrent densities ranging from 30-200 mA/cm². This type of porosity isachieved since the epilayer 12 initially had a doping level on the rangeof 10¹⁸ cm⁻³ to 10¹⁹ cm⁻³. The anodizing layer is described in E. J.Zorinsky, D. D. Spratt, R. L. Virkus, "The `Islands` Method --AManufacturable Porous Silicon SOI Technology", Technical Digest,International Electron Devices Meeting, Los Angeles, Dec. 7-10, 1986,which is hereby incorporated by reference.

Referring now to FIG. 5, after converting the anodizable layer 12 to aporous film 12', the porous film s converted by oxidation to SIO₂ aslayer 13. This results in an SiO₂ underlayer 13 formed without a changein volume from that of the original layer 12, which is advantageous inpreventing stress and deformation of the ridge. The oxidation isperformed by subjecting the surface to a high temperature andpressurized oxidizing ambient. In this process, a small amount ofoxidation has simultaneously occurred on the sidewalls of the ridges toform sidewall oxide layers 13'. Simultaneous oxidation of the top sidehas been prevented by the masking film 16. After the removal of 16,another oxidation is performed to extend the SiO₂ sidewall over the topsof the ridges 14. Oxidation of tops and sidewalls in separate stepshelps maintain the desired rectangular shape of the silicon core, whileproviding a thermal oxide cladding completely around the silicon cores.

After formation of the sidewall oxide layers 13', a dielectric back filllayer 18 is deposited on the substrate in between the ridge channels 14.This results in a thicker cladding on the upper surfaces and sidesurfaces without further consumption of the core.

Referring now to FIG. 7, there is illustrated a perspective view of thestructure of FIG. 6. It can be seen in FIG. 7 that the ridge channels 14are longitudinal in shape and form waveguides, with silicon cores 14,which are the propagating media, silicon oxide cladding 13 and 13', andsilicon dioxide as an additional dielectric layer 18. To preventradiative noise or stray signals from refracting into the waveguides, itis necessary to cover the structure shown with an opaque material.Access to a waveguide, for purposes of input or extraction of radiation,is accomplished by either juxtaposing a coupling structure to an exposedcore end or selectively exposing the core on the top or sides, as byetching through the dielectric layers. Access to the waveguides can bemade by either selective removal of oxide or coupling to exposed siliconends.

For a given wavelength of light to be transmitted in a waveguide, thecross-sectional dimensions of the core 14 and the thickness of thecladding 13 depend on the propagation modes chosen and the degree ofconfinement required. For example, at the standard telecommunicationswavelength of 1.3 um, the refractive indices of silicon, 3.5, andsilicon dioxide, 1.5, impose a TE monomode cutoff of approximately 0.21um. In other words, in applications that require single modepropagation, the vertical dimension of the core 14 cannot exceed 0.21um. In applications where multimode propagation is allowed or required,the vertical dimension of the core can be or will be greater than 0.21um.

At a thickness of 0.21 um, the confinement factor, i.e., the fraction ofthe electric field of the light wave contained in the core, isapproximately 0.85. The remaining 15% of the electric field existsoutside the core in an exponentially decaying, lossless, evanescentmode. It is important that very little of the electric field extend tothe substrate 10, whereupon it contributes to leakage loss of power. Thethickness of cladding layer 13 required to reduce the electric fieldintensity at the layer 13 and substrate 10 boundary to 1% of maximum isapproximately 0.34 um. As the vertical dimension of the core is reducedbelow 0.21 um, the confinement factor is also reduced, and the thicknessof layer 13 must increase to satisfy the same leakage criteria. In thecase of longer-wavelength single-mode light propagation, the maximumvertical dimension of the core 14 is greater, but the evanescent modeintensity falls of more gradually in the cladding, so a thicker layer 13is required. For example, at the wavelength 3.0 um, the maximumthickness of the core 14 is approximately 0.47 um, and the thickness ofthe cladding 13 required to meet the leakage criterion chosen above is0.76 um.

Although the preferred embodiment has been described in detail, itshould be understood that various changes, substitutions and alterationscan be made therein without departing from the spirit and scope of theinvention as defined by the appended claims.

I claim:
 1. The method for fabricating a semiconductor waveguide,comprising:providing a semiconductor substrate having a low or intrinsiclevel of dopant impurities; forming a first layer of semiconductormaterial over one surface of the semiconductor substrate to apredetermined thickness; forming a second layer of semiconductormaterial on the upper surface of the first layer of semiconductormaterial; etching the second layer of semiconductor material to form atleast one ridge that functions as an optical waveguide and having atleast a lower surface adjacent the upper surface of the first layer ofsemiconductor material; porifying the first layer of semiconductormaterial; and converting the first layer of semiconductor material tosilicon dioxide.